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๐Ÿ”—Statics and Strength of Materials Unit 7 Review

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7.2 Normal and shear strain

๐Ÿ”—Statics and Strength of Materials
Unit 7 Review

7.2 Normal and shear strain

Written by the Fiveable Content Team โ€ข Last updated September 2025
Written by the Fiveable Content Team โ€ข Last updated September 2025
๐Ÿ”—Statics and Strength of Materials
Unit & Topic Study Guides

Normal and shear strain are crucial concepts in understanding material deformation. Normal strain measures length changes along the force direction, while shear strain quantifies angular deformation perpendicular to the force. These concepts are fundamental to analyzing how materials respond to different types of stress.

Calculating strain involves simple formulas that relate changes in length or angle to original dimensions. Understanding these calculations helps engineers predict and design for material behavior under various loading conditions. This knowledge is essential for ensuring structures and components can withstand applied forces without failure.

Normal vs Shear Strain

Definition and Characteristics

  • Normal strain is the change in length of a material in the direction of the applied force divided by its original length
    • Represents the elongation or contraction of a material along the axis of loading
  • Shear strain is the angular deformation or change in shape of a material subjected to shear stress
    • Defined as the tangent of the angle of deformation
    • Represents the distortion of a material perpendicular to the axis of loading

Key Differences

  • The key difference between normal strain and shear strain is the direction of deformation relative to the applied force
    • Normal strain occurs parallel to the force
    • Shear strain occurs perpendicular to the force
  • Normal strain causes a change in the length of the material without a change in its shape
    • Example: A rubber band stretching when pulled
  • Shear strain causes a change in the shape of the material without a change in its volume
    • Example: A deck of cards deforming into a parallelogram when pushed from the side

Strain Calculation

Normal Strain Formula

  • Normal strain (ฮต) is calculated using the formula: ฮต=(Lโˆ’L0)/L0ฮต = (L - Lโ‚€) / Lโ‚€
    • $L$ is the final length
    • $Lโ‚€$ is the initial length of the material
  • Example: If a steel bar with an initial length of 1 m elongates to 1.001 m under tension, the normal strain is (1.001 - 1) / 1 = 0.001 or 0.1%

Shear Strain Formula

  • Shear strain (ฮณ) is calculated using the formula: ฮณ=tan(ฮธ)ฮณ = tan(ฮธ)
    • $ฮธ$ is the angle of deformation
  • In some cases, shear strain can also be calculated using the formula: ฮณ=ฮ”x/yฮณ = ฮ”x / y
    • $ฮ”x$ is the transverse displacement
    • $y$ is the perpendicular distance from the fixed end
  • Example: If a rectangular block deforms by an angle of 2ยฐ under shear stress, the shear strain is tan(2ยฐ) โ‰ˆ 0.035 or 3.5%

Consistency in Units

  • It is important to ensure that the units of measurement for length and displacement are consistent when calculating strains
    • Example: If the initial length is in meters, the final length should also be in meters

Strain and Deformation

Normal Strain Deformation

  • Normal strain can be illustrated by a rectangular bar subjected to a tensile or compressive force along its longitudinal axis
    • The bar will elongate under tension or contract under compression
    • The cross-sectional shape remains unchanged
  • Example: A concrete column shortening under the weight of a building

Shear Strain Deformation

  • Shear strain can be illustrated by a rectangular block subjected to a shear force parallel to one of its faces
    • The block will deform into a parallelogram shape
    • The angle between the deformed and original faces represents the shear strain
  • Example: A book on a shelf tilting when pushed from the side

Exaggeration in Illustrations

  • In both cases, the deformation is typically exaggerated in illustrations to clearly demonstrate the strain effects
    • The actual deformations in engineering materials are often small
  • Combining normal and shear strains can result in more complex deformations
    • Example: Simultaneous elongation and distortion of a material under a combined loading scenario

Stress and Strain in Materials

Definitions

  • Stress is the internal force per unit area acting on a material
  • Strain is the deformation or change in shape of the material in response to the applied stress

Hooke's Law

  • Hooke's law states that, within the elastic limit, stress is directly proportional to strain
    • The constant of proportionality is known as the modulus of elasticity (E) for normal stress and strain
    • The constant of proportionality is known as the shear modulus (G) for shear stress and strain
  • The relationship between normal stress (ฯƒ) and normal strain (ฮต) is given by: ฯƒ=Eร—ฮตฯƒ = E ร— ฮต
    • $E$ is the modulus of elasticity
  • The relationship between shear stress (ฯ„) and shear strain (ฮณ) is given by: ฯ„=Gร—ฮณฯ„ = G ร— ฮณ
    • $G$ is the shear modulus

Elastic Limit and Plastic Deformation

  • The elastic limit is the maximum stress a material can withstand without experiencing permanent deformation
    • Within the elastic limit, the material will return to its original shape when the load is removed
  • Beyond the elastic limit, the material undergoes plastic deformation
    • The stress-strain relationship becomes nonlinear
    • The material will not return to its original shape when the load is removed
  • Example: A metal paperclip bending and retaining its new shape after being deformed

Stress-Strain Curve

  • The stress-strain curve is a graphical representation of the relationship between stress and strain for a given material
    • Helps engineers understand the material's behavior under various loading conditions
  • The curve typically includes the elastic region, yield point, plastic region, and ultimate strength point
    • Example: A stress-strain curve for a ductile material like mild steel